Inlining everything

CliMA · Jan 22, 2024 · 492967a · 492967a
1 parent dd73501
commit 492967a
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Showing 6 changed files with 357 additions and 301 deletions.
diff --git a/src/Parameters.jl b/src/Parameters.jl
@@ -56,20 +56,20 @@ Base.eltype(::ThermodynamicsParameters{FT}) where {FT} = FT
 
 # wrappers
 for fn in fieldnames(ATP)
-    @eval $(fn)(ps::ATP) = ps.$(fn)
+    @eval @inline $(fn)(ps::ATP) = ps.$(fn)
 end
 
 # Derived parameters
-R_d(ps::ATP) = ps.gas_constant / ps.molmass_dryair
-R_v(ps::ATP) = ps.gas_constant / ps.molmass_water
-molmass_ratio(ps::ATP) = ps.molmass_dryair / ps.molmass_water
-LH_f0(ps::ATP) = ps.LH_s0 - ps.LH_v0
-e_int_v0(ps::ATP) = ps.LH_v0 - R_v(ps) * ps.T_0
-e_int_i0(ps::ATP) = LH_f0(ps)
-cp_d(ps::ATP) = R_d(ps) / ps.kappa_d
-cv_d(ps::ATP) = cp_d(ps) - R_d(ps)
-cv_v(ps::ATP) = ps.cp_v - R_v(ps)
-cv_l(ps::ATP) = ps.cp_l
-cv_i(ps::ATP) = ps.cp_i
+@inline R_d(ps::ATP) = ps.gas_constant / ps.molmass_dryair
+@inline R_v(ps::ATP) = ps.gas_constant / ps.molmass_water
+@inline molmass_ratio(ps::ATP) = ps.molmass_dryair / ps.molmass_water
+@inline LH_f0(ps::ATP) = ps.LH_s0 - ps.LH_v0
+@inline e_int_v0(ps::ATP) = ps.LH_v0 - R_v(ps) * ps.T_0
+@inline e_int_i0(ps::ATP) = LH_f0(ps)
+@inline cp_d(ps::ATP) = R_d(ps) / ps.kappa_d
+@inline cv_d(ps::ATP) = cp_d(ps) - R_d(ps)
+@inline cv_v(ps::ATP) = ps.cp_v - R_v(ps)
+@inline cv_l(ps::ATP) = ps.cp_l
+@inline cv_i(ps::ATP) = ps.cp_i
 
 end
diff --git a/src/Thermodynamics.jl b/src/Thermodynamics.jl
@@ -65,10 +65,10 @@ const APS = TP.ThermodynamicsParameters
 # Error on convergence must be the default
 # behavior because this can result in printing
 # very large logs resulting in CI to seemingly hang.
-error_on_non_convergence() = true
+@inline error_on_non_convergence() = true
 
 # Allow users to skip printing warnings on non-convergence
-print_warning() = true
+@inline print_warning() = true
 
 @inline q_pt_0(::Type{FT}) where {FT} = PhasePartition(FT(0), FT(0), FT(0))
 

diff --git a/src/config_numerical_method.jl b/src/config_numerical_method.jl
@@ -5,7 +5,7 @@
 
 # KA.@print only accepts literal strings, so we must
 # branch to print which method is being used.
-function print_numerical_method(
+@inline function print_numerical_method(
     ::Type{sat_adjust_method},
 ) where {sat_adjust_method}
     if sat_adjust_method <: RS.NewtonsMethod
@@ -21,7 +21,7 @@ function print_numerical_method(
     end
 end
 
-function print_T_guess(
+@inline function print_T_guess(
     ::Type{sat_adjust_method},
     T_guess::Real,
 ) where {sat_adjust_method}
@@ -32,7 +32,7 @@ function print_T_guess(
     end
 end
 
-function print_T_guess(
+@inline function print_T_guess(
     ::Type{sat_adjust_method},
     T_guess::Nothing,
 ) where {sat_adjust_method}
@@ -46,7 +46,7 @@ end
 #####
 ##### Thermodynamic variable inputs: ρ, e_int, q_tot
 #####
-function sa_numerical_method(
+@inline function sa_numerical_method(
     ::Type{NM},
     param_set::APS,
     ρ::FT,
@@ -64,7 +64,7 @@ function sa_numerical_method(
     return RS.NewtonsMethod(T_init)
 end
 
-function sa_numerical_method(
+@inline function sa_numerical_method(
     ::Type{NM},
     param_set::APS,
     ρ::FT,
@@ -82,7 +82,7 @@ function sa_numerical_method(
     return RS.NewtonsMethodAD(T_init)
 end
 
-function sa_numerical_method(
+@inline function sa_numerical_method(
     ::Type{NM},
     param_set::APS,
     ρ::FT,
@@ -99,7 +99,7 @@ function sa_numerical_method(
     return RS.SecantMethod(T_1, T_2)
 end
 
-function sa_numerical_method(
+@inline function sa_numerical_method(
     ::Type{NM},
     param_set::APS,
     ρ::FT,
@@ -120,7 +120,7 @@ end
 ##### Thermodynamic variable inputs: ρ, p, q_tot
 #####
 
-function sa_numerical_method_ρpq(
+@inline function sa_numerical_method_ρpq(
     ::Type{NM},
     param_set::APS,
     ρ::FT,
@@ -138,7 +138,7 @@ function sa_numerical_method_ρpq(
     return RS.NewtonsMethodAD(T_init)
 end
 
-function sa_numerical_method_ρpq(
+@inline function sa_numerical_method_ρpq(
     ::Type{NM},
     param_set::APS,
     ρ::FT,
@@ -157,7 +157,7 @@ end
 ##### Thermodynamic variable inputs: p, e_int, q_tot
 #####
 
-function sa_numerical_method_peq(
+@inline function sa_numerical_method_peq(
     ::Type{NM},
     param_set::APS,
     p::FT,
@@ -175,7 +175,7 @@ function sa_numerical_method_peq(
     return RS.NewtonsMethodAD(T_init)
 end
 
-function sa_numerical_method_peq(
+@inline function sa_numerical_method_peq(
     ::Type{NM},
     param_set::APS,
     p::FT,
@@ -196,7 +196,7 @@ end
 ##### Thermodynamic variable inputs: p, h, q_tot
 #####
 
-function sa_numerical_method_phq(
+@inline function sa_numerical_method_phq(
     ::Type{NM},
     param_set::APS,
     p::FT,
@@ -217,7 +217,7 @@ function sa_numerical_method_phq(
     return RS.NewtonsMethodAD(T_init)
 end
 
-function sa_numerical_method_phq(
+@inline function sa_numerical_method_phq(
     ::Type{NM},
     param_set::APS,
     p::FT,
@@ -237,7 +237,7 @@ function sa_numerical_method_phq(
     return RS.SecantMethod(T_1, T_2)
 end
 
-function sa_numerical_method_phq(
+@inline function sa_numerical_method_phq(
     ::Type{NM},
     param_set::APS,
     p::FT,
@@ -261,7 +261,7 @@ end
 ##### Thermodynamic variable inputs: p, θ_liq_ice, q_tot
 #####
 
-function sa_numerical_method_pθq(
+@inline function sa_numerical_method_pθq(
     ::Type{NM},
     param_set::APS,
     p::FT,
@@ -272,14 +272,14 @@ function sa_numerical_method_pθq(
 ) where {FT, NM <: RS.RegulaFalsiMethod, phase_type <: PhaseEquil}
     _T_min::FT = TP.T_min(param_set)
     _T_max::FT = TP.T_max(param_set)
-    air_temp(q) = air_temperature_given_pθq(param_set, p, θ_liq_ice, q)
+    @inline air_temp(q) = air_temperature_given_pθq(param_set, p, θ_liq_ice, q)
     T_1 = max(_T_min, air_temp(PhasePartition(q_tot))) # Assume all vapor
     T_2 = T_1 + 10
     T_1 = T_1 - 10
     return RS.RegulaFalsiMethod(T_1, T_2)
 end
 
-function sa_numerical_method_pθq(
+@inline function sa_numerical_method_pθq(
     ::Type{NM},
     param_set::APS,
     p::FT,
@@ -289,14 +289,14 @@ function sa_numerical_method_pθq(
     T_guess::Union{FT, Nothing},
 ) where {FT, NM <: RS.SecantMethod, phase_type <: PhaseEquil}
     _T_min::FT = TP.T_min(param_set)
-    air_temp(q) = air_temperature_given_pθq(param_set, p, θ_liq_ice, q)
+    @inline air_temp(q) = air_temperature_given_pθq(param_set, p, θ_liq_ice, q)
     T_1 = max(_T_min, air_temp(PhasePartition(q_tot))) # Assume all vapor
     T_2 = air_temp(PhasePartition(q_tot, FT(0), q_tot)) # Assume all ice
     T_2 = bound_upper_temperature(T_1, T_2)
     return RS.SecantMethod(T_1, T_2)
 end
 
-function sa_numerical_method_pθq(
+@inline function sa_numerical_method_pθq(
     ::Type{NM},
     param_set::APS,
     p::FT,
@@ -306,7 +306,7 @@ function sa_numerical_method_pθq(
     T_guess::Union{FT, Nothing},
 ) where {FT, NM <: RS.NewtonsMethodAD, phase_type <: PhaseEquil}
     T_min::FT = TP.T_min(param_set)
-    air_temp(q) = air_temperature_given_pθq(param_set, p, θ_liq_ice, q)
+    @inline air_temp(q) = air_temperature_given_pθq(param_set, p, θ_liq_ice, q)
     T_init = if T_guess isa Nothing
         max(T_min, air_temp(PhasePartition(q_tot))) # Assume all vapor
     else

diff --git a/src/isentropic.jl b/src/isentropic.jl
@@ -22,7 +22,7 @@ The air pressure for an isentropic process, where
  - `θ` potential temperature
  - `Φ` gravitational potential
 """
-function air_pressure_given_θ(
+@inline function air_pressure_given_θ(
     param_set::APS,
     θ::FT,
     Φ::FT,
@@ -44,7 +44,7 @@ The air pressure for an isentropic process, where
  - `T∞` ambient temperature
  - `p∞` ambient pressure
 """
-function air_pressure(
+@inline function air_pressure(
     param_set::APS,
     T::FT,
     T∞::FT,
@@ -64,7 +64,7 @@ The air temperature for an isentropic process, where
  - `p` pressure
  - `θ` potential temperature
 """
-function air_temperature(
+@inline function air_temperature(
     param_set::APS,
     p::FT,
     θ::FT,